Sampling Theorem: A Comprehensive Overview Introduction
HODECEDSIET
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10 slides
Jul 28, 2024
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About This Presentation
The Sampling Theorem, also known as the Nyquist-Shannon Sampling Theorem, is a fundamental concept in the field of digital signal processing and communications. It provides a formal framework for understanding how continuous-time signals can be sampled and reconstructed without loss of information. ...
The Sampling Theorem, also known as the Nyquist-Shannon Sampling Theorem, is a fundamental concept in the field of digital signal processing and communications. It provides a formal framework for understanding how continuous-time signals can be sampled and reconstructed without loss of information. The theorem has wide applications in various domains, including telecommunications, audio processing, medical imaging, and more. This comprehensive overview aims to explore the principles, implications, and applications of the Sampling Theorem in detail.
Historical Background
The roots of the Sampling Theorem can be traced back to the work of Harry Nyquist and Claude Shannon. Harry Nyquist, in his 1928 paper, laid the groundwork for understanding the constraints on signal transmission. Claude Shannon, in his seminal 1948 paper "A Mathematical Theory of Communication," formalized these concepts and extended them to the domain of digital communication.
Theoretical Foundation
Continuous-Time Signals
A continuous-time signal,
π₯
(
π‘
)
x(t), is a function of time that can take any value at any point in time. Such signals are ubiquitous in the real world, representing various physical phenomena like sound waves, temperature variations, and more.
Discrete-Time Signals
A discrete-time signal,
π₯
[
π
]
x[n], is a sequence of values obtained by sampling a continuous-time signal at specific intervals. This process of converting a continuous-time signal into a discrete-time signal is known as sampling.
The Sampling Process
The sampling process can be mathematically represented as:
π₯
π
(
π‘
)
=
π₯
(
π‘
)
β
β
π
=
β
β
β
πΏ
(
π‘
β
π
π
)
x
s
β
(t)=x(t)β β
n=ββ
β
β
Ξ΄(tβnT)
where
π
T is the sampling period and
πΏ
(
π‘
)
Ξ΄(t) is the Dirac delta function. This operation effectively "picks" the values of
π₯
(
π‘
)
x(t) at intervals of
π
T, resulting in a discrete-time signal.The Sampling Theorem
The Sampling Theorem states that a bandlimited continuous-time signal can be perfectly reconstructed from its samples if the sampling frequency is greater than twice the highest frequency component of the signal. Mathematically, if
π₯
(
π‘
)
x(t) is a bandlimited signal with a maximum frequency
π
π
π
π₯
f
max
β
, then the sampling frequency
π
π
f
s
β
must satisfy:
π
π
>
2
π
π
π
π₯
f
s
β
>2f
max
β
This critical frequency,
2
π
π
π
π₯
2f
max
β
, is known as the Nyquist rate.
Proof of the Sampling Theorem
The proof of the Sampling Theorem involves several steps:
Fourier Transform of the Signal: The Fourier Transform of
π₯
(
π‘
)
x(t) gives us its frequency representation
π
(
π
)
X(f).
Fourier Transform of the Sampled Signal: The Fourier Transform of the sampled signal
π₯
π
(
π‘
)
x
s
β
(t) results in a periodic repetition of
π
(
π
)
X(f) with a period of
π
π
f
s
β
.
Condition for Perfect Reconstruction: If
π
π
>
2
π
π
π
π₯
f
s
β
>2f
max
β
, the replicas of
π
(
π
)
X(f) do not overlap, allowing for the ori
Size: 256.32 KB
Language: en
Added: Jul 28, 2024
Slides: 10 pages
Slide Content
Sampling Process
Sampling Theorem (Third phase) A bandlimited signal can be reconstructed exactly if it is sampled at a rate at least twice of the maximum frequency component present in the signal ( fs > 2f m). Sampled analog waveform t T s T s m(t) t Sampler Product modulator t T s 2T s 3T s -T s -2T s 1
Continued⦠Fourier series representation of train impulse signal is given as: b n = 0; because train impulse signal is an even signal
Continuedβ¦ Spectrum m (t) f m -f m Modulation by cos ( ο· s t) Modulation by cos (2 ο· s t)
Continuedβ¦ Spectrum w s - w s Spectrum f m -f m f s -f m f s - f s fs+ f m - fs+ f m - fs+ f m β¦ β¦
Continuedβ¦ f m -f m f s -f m f s - f s fs+ f m - fs+ f m - fs+ f m β¦ β¦ Gaurd band Gaurd band = GB= fs β f m β f m = fs β 2f m There are basically three different cases on guard band; GB = 0 fs = 2f m GB > 0 fs > 2f m GB < 0 fs < 2f m
Continued⦠Ideal condition, practically message can not be recover back Case 1. fs = 2f m Nyquist Rate ⦠⦠Case 2. fs > 2f m Over sampling Full reconstruction of message signal is possible in this case ⦠⦠Ideal filter Practical filter Ideal filter Practical filter
Continued⦠⦠⦠Case 3. fs < 2f m Aliasing effect Interference of high frequency components Recovery of original message signal is not possible Ideal filter Practical filter
Applications Audio sampling Video sampling Communication systems Digital signal processing Speech sampling 3D sampling Digital Storage Oscilloscope (DSO)